Carlson
Alexander
a,
James A.
Thom
a,
Alan M.
Kenwright
b,
Kirsten E.
Christensen
a,
Thomas Just
Sørensen
ac and
Stephen
Faulkner
*a
aChemistry Research Laboratory, Department of Chemistry, University of Oxford, 12 Mansfield Road, Oxford, OX1 3TA, UK. E-mail: stephen.faulkner@chem.ox.ac.uk
bDepartment of Chemistry, University of Durham, South Road, Durham DH1 3LE, UK
cNano-Science Centre and Department of Chemistry, University of Copenhagen, 2100 København Ø, Denmark
First published on 27th December 2022
Halide recognition by supramolecular receptors and coordination complexes in water is a long-standing challenge. In this work, we report chloride binding in water and in competing media by pre-organised binuclear kinetically inert lanthanide complexes, bridged by flexible –(CH2)2– and –(CH2)3– spacers, forming [Ln2(DO3A)2C-2] and [Ln2(DO3A)2C-3], respectively. These hydrophilic, neutral lanthanide coordination complexes are shown to bind chloride with apparent association constants of up to 105 M−1 in water and in buffered systems. Hydroxide bridging was observed in these complexes at basic pH, which was proven to be overcome by chloride. Thus, these lanthanide complexes show promise towards chloride recognition in biology and beyond. The results described here have clearly identified a new area of anion coordination chemistry that is ripe for detailed exploration.
Nature provides inspiration towards anion binding: protein-based interactions include bacterial sulfate binding protein and phosphatase enzymes, which selectively recognise sulfate and phosphate under physiological conditions via a network of hydrogen bonds from neutral donors. In these proteins, anion affinity is increased by a hydrophobic environment providing complementarity of charge and a shape that minimises the receptor desolvation energy.6 These interactions have inspired biomimetic receptors that integrate additional binding sites within the synthetic host, creating a structured binding pocket with high geometric complementarity.1,3–5 A range of interactions such as the macrocyclic effect,1,2 and conventional ion-pairing have been exploited in anion recognition;5a the latter based on electrostatics,1 and supported by hydrogen bonding,2 halogen bonding,7 anion–π interactions,8 and coordinate bond using Lewis acids such as metals.3,4
Here, we focus on chloride binding. Chloride is the most abundant physiological anion9 and plays important roles in neuronal growth (104–115 mM in extracellular fluid),10 and development of the central nervous system (115–130 mM in cerebrospinal fluid) through the functions of chloride channels. The intracellular chloride concentration (up to 70 mM in eukaryotic cell types) is crucial in moderating neuronal excitability and neurotransmission.11 Tracking chloride in living systems is vital if we are to understand diseases related to chloride transport defects such as cystic fibrosis and epilepsy.9,11,12 Apart from its importance as the counterion of life,9,12 sequestering salt from sea water (559 mM of chloride in surface sea water)13 for clean drinking water is an ongoing challenge.14 However, developing suitably selective receptors for chloride in water continues to be a challenge.1,4,5,15
The large enthalpy and free energy of hydration of halides (Table 1) make chloride recognition challenging in water.16d Halide anions exhibit different levels of hydration in different solvents as reflected by the Hofmeister series of anion hydrophobicity.17 Across the series,§ the decrease in charge density results in increasing lipophilicity and weaker hydration.7 However, the solvation of the host must also be considered in designing an effective receptor for anion recognition.1,3–5
Anion | Radius (Å) | n hyd | −ΔG°hyd (kJ mol−1) | −ΔH°hyd (kJ mol−1) |
---|---|---|---|---|
HO− | 1.33 | 2.7 | 430 | 520 |
F− | 1.33 | 2.7 | 465 | 510 |
Cl− | 1.81 | 2 | 340 | 367 |
Br− | 1.96 | 1.8 | 315 | 336 |
I− | 2.2 | 1.6 | 275 | 291 |
The extent of solvation of the host, guest, and supramolecular assemblies depends on the solvent. Polar protic solvents such as water and methanol strongly solvate charged species, forming hydrogen bonds with both the anion and the host molecule.1,5 By contrast, in less polar aprotic solvents such as dichloromethane, the anion is weakly solvated and neutral receptors are able to function.5,17 Strong electrostatic or metal–ligand interactions offer the potential to overcome the anion hydration energy and allow binding in biological media.3,4
We previously reported a lanthanide tethered rotaxane that binds to chloride in apolar media (Fig. 1b). In this, the first binding of chloride involves chelation to the metal, a second binding event occurs by encapsulation within the rotaxane.18 Gale, Davis et al. have reported cholapods made of a steroidal framework containing squaramide groups in axial positions which bind to chloride and other anions of tetraethylammonium salts with ∼1014 M−1 affinity in wet chloroform, employing a variation of Cram's extraction procedure.19 Flood et al. have reported a triazolo cage which binds to chloride with ∼1017 M−1 affinity in dichloromethane, which is very effective in sequestering chloride from water and has been shown to prevent brine-accelerated corrosion when coated onto mild steel (Fig. 1a).20 Beer et al. have designed rotaxane hosts based on iodotriazole halogen bonding and amide hydrogen bonding with the halogens, but it recognises iodide (Ka = 2200 M−1) better than chloride (Ka = 55 M−1) and bromide in water.21 Other chloride binding supramolecular agents have been extensively reviewed elsewhere.1,5,15
Fig. 1 Cartoon illustration of receptors that recognise chloride. (a) Receptor that extracts chloride from water to dichloromethane (adapted from ref. 20). (b) Receptor that binds to chloride in mixed media (dichloromethane and methanol) (adapted from ref. 18). (c) Our receptor that binds to chloride in water. |
Lanthanide complexes are an attractive choice for developing anion receptors due to their ability to report anion binding by MRI, luminescence, and optical imaging.22 The luminescence applications use lanthanide complexes as luminescent tags, exploiting stable complexes in which their luminescence signal is enhanced via the antenna principle where chromophores sensitise lanthanide luminescence and overcome the inherently low molar absorption coefficients associated with f–f transitions.22,23 Furthermore, the necessity for kinetic stability in clinical use ensures that macrocyclic ligands related to DOTA are well understood in competitive media with high anion concentrations.4,22,23 In such systems, anion chelation is achievable on the metal site without the dissociation of the lanthanide complex.4
Anion recognition by lanthanide complexes can reflect either collisional quenching of excited states by anions,24 or anion binding.4 While luminescence can be modulated both by collision and anion binding, the latter generates a ‘turn-off’ event in MRI since the functioning of MRI contrast agents requires the presence of water molecules in the inner-coordination sphere which exchange with the bulk water.24 Thus, isostructural MRI and luminescent probes can be constructed with suitable lanthanide ions for targeted anion binding thereby allowing one design platform to exploit bio-imaging combining paramagnetism and luminescence, an exclusive feature offered by the lanthanides.4,22 Halides are strong Lewis bases which coordinate to metals that are hard Lewis acids.25 Using this HSAB approach, several mononuclear Ln(III) complexes comprising cryptands,26 and cyclen derived C2 (ref. 27) and C4 symmetric28,29 ligands have been reported to chelate fluoride at the metal centre, but none have been reported to bind chloride in water.
Binuclear lanthanide(III) complexes of two heptadentate DO3A-based binding domains tethered by aryl spacers were studied for binding organic dicarboxylate anions at physiological pH;30 sensing biologically relevant anions such as phosphate, methylphosphate, double-stranded DNA and a DNA hairpin loop;31 and as a pH sensor.32 We have explored this binuclear approach by incorporating kinetically inert charge neutral lanthanide DO3A centres bridged by different m-xylyl scaffolds to achieve reversible binding of dinicotinate and isophthalate guests with high affinity at physiological conditions, but this requires methanol to improve the solvation of these guests.33
In this work, we report how binuclear complexes can be tailored to bind chloride ions in water under conditions where mononuclear complexes4,26–30 and free lanthanide ions34 do not interact with chloride. We hypothesised that coordinatively unsaturated neutral binuclear lanthanide(III) complexes of DO3A ligands bridged by ethane and propane linkers ([Ln2(DO3A)2C-2] and [Ln2(DO3A)2C-3]) would create a pre-organised pocket between the metal centres capable of hosting halides coordinated to the lanthanide metal centres. Furthermore, having a short and flexible spacer between the coordinatively unsaturated hard Lewis acids, which act as acceptors would increase the steric strain thereby limiting their conformational freedom,35 where subsequent halide binding would lead to a smaller entropy loss in the host. Both binuclear complexes respond to halides under physiological conditions and the binding can be followed by luminescence and NMR spectroscopy. A neutral mononuclear lanthanide propargyl DO3A complex [Ln(pDO3A)] was23 used to compare the relative effectiveness of mononuclear complexes.
Scheme 1 Synthetic scheme of proposed binuclear complexes. The mononuclear complex used as a model system is shown inside the black box. |
These kinetically robust binuclear complexes23 exhibit variations in behaviour with pH. At neutral pH, the 1H NMR spectra of the paramagnetic Eu(III) and Yb(III) complexes consist of broad lines; however, at pD 10.12, the lines are sharp and well defined (Fig. S28, S31, S34, and S36‡). This observation can be explained by the rapid inter-conversion between diastereomeric forms of the compound, in which the coordination environment at the lanthanide centre varies between Square Antiprism (SAP) and Twisted Square Antiprism (TSAP) geometries. At high pH, interchange between these species was found to be slow on the NMR timescale, resulting in sharp spectral lines. Furthermore, luminescence spectra of [Eu2(DO3A)2C-2] and [Eu2(DO3A)2C-3] at pH 4 and 7 showed no significant change (Fig. S62–S65‡), but at pH 9.9, the form and shape of the emission spectra was changed, which implies hydroxide binding to the metal centres. A decrease in the hydration number of the complexes can be inferred from luminescence lifetime measurements at increasing pH (Fig. S112 and S115; Tables S1 and S4‡). These results complement the NMR observations that chelation to hydroxide is observed at basic pH.
Chloride binding by the binuclear Eu(III) complexes were then explored. Steady-state luminescence titrations were performed in deionised water, phosphate buffer at pH 7.4, and in CHES buffer at pH 9.9. In the case of deionised water and in phosphate buffer, the emission intensity decreased with increasing KCl addition, but the opposite was the case in CHES buffer (Fig. 2, S74–S78 and S94–S99‡). It should be noted that chloride can act as a PeT quencher, reducing the observed lanthanide centred emission intensity.24 However, a single binding event (K1) was observed in all three cases and the binding strength increased as we move into buffered systems (Table 2). These results could be suggestive of competitive binding of phosphate: indeed, the changes to the form of the spectra in phosphate buffer (in comparison with the spectra in water) are strongly suggestive of phosphate binding in line with other mono and binuclear lanthanide complexes derived from DO3A.4,31,37
Fig. 2 Chloride chelation by the binuclear complexes in water. (a) Structural representation of the binding events in water. (b) 49 MHz 35Cl NMR titration spectra of 0.035 M [Tb2(DO3A)2C-3] with increasing additions of KCl (stock concentration, 1.4 M) in D2O at 298 K (Fig. S52 for binding isotherm‡). Each spectrum was recorded with a capillary tube insert containing saturated KCl in D2O (δ = 0 ppm) (non-dilution method used). (c) Steady-state luminescence titration spectra of 1 mM [Eu2(DO3A)2C-2] (λex = 393 nm) against KCl (stock concentration, 0.02 M) in 0.01 M CHES buffer (pH 9.98) at 22 °C; spectrum of neat complex solution (), spectra upon the additions of KCl (grey), spectrum upon the final addition of KCl () (non-dilution method used). The inset expands the ΔJ = 0 and ΔJ = 1 emission bands (Fig. S78 for binding isotherm‡). (d) Normalised emission trend of ΔJ = 2/ΔJ = 1 obtained from steady-state emission titrations for 1 mM [Eu2(DO3A)2C-2] against KCl in deionised water, 0.01 M phosphate buffer (pH 7.4), and 0.01 M CHES buffer (pH 9.9) at 22 °C. (e) Normalised model of speciation obtained from ΔJ = 2/ΔJ = 1 bands from steady-state emission titration spectra of [Eu2(DO3A)2C-2] against KCl in 0.01 M CHES buffer (pH 9.9) at 22 °C. |
Halide | Mediab | Binding constant (K in M−1)c,d | |
---|---|---|---|
[Eu2(DO3A)2C-2] | [Eu2(DO3A)2C-2] | ||
a The binding of halides with the complexes were studied by steady-state luminescence titrations with varying concentration of potassium halides (non-dilution method used) and binding isotherm generated using DYNAFIT®. b All buffers were maintained at 0.01 M in deionised water: PBS = phosphate buffer saline at pH 7.4; PB = phosphate buffer at pH 7.4; CHES = N-cyclohexyl-2-aminoethanesulfonic acid at pH 9.98; Tris–HCl = tris(hydroxymethyl)aminomethane hydrochloride at pH 7.4. c K 1 = first binding event; K2 = second binding event; K3 = third binding event – deduced from binding isotherm generated using DYNAFIT®. d ± is the coefficient of variation in percentage for each binding event obtained from binding isotherm plotted in DYNAFIT® by employing trust-region algorithm in confidence interval at 95% probability level. Confidence intervals for all binding constants are given in the ESI under each binding isotherm. | |||
Cl− | Water | K 1 = 2800 (±7%) | K 1 = 4550 (±3.9%) |
PB | K 1 = 9400 (±12.2%) | K 1 = 6640 (±7.3%) | |
CHES | K 1 = 7460 (±11.2%) | K 1 = 12210 (±7%) | |
F− | Water | K 1 = 600000 (±39.7%) | K 1 = 10480 (±5.9%) |
K 2 = 144000 (±33.5%) | K 2 = 10950 (±4%) | ||
K 3 = 394.7 (±2.3%) | K 3 = 6570 (±3.6%) | ||
Methanol | K 1 = 54800 (±11.8%) | K 1 = 179000 (±13.2%) | |
K 2 = 20200 (±10.6%) | K 2 = 32000 (±13%) | ||
K 3 = 0.002843 (±0.6%) | K 3 = 728 (±7.5%) | ||
PBS | K 1 = 4030 (±2.9%) | K 1 = 5350 (±6.9%) | |
K 2 = 18.57 (±1%) | |||
Tris–HCl | K 1 = 106000 (±38.9%) | K 1 = 1670 (±14.7%) | |
K 2 = 219.1 (±0.8%) | K 2 = 116.4 (±1.7%) | ||
CHES | K 1 = 13600 (±9.9%) | K 1 = 3840 (±9.6%) | |
K 2 = 3494 (±2.8%) |
NMR studies of chloride binding at lanthanide centres present difficulties due to the interference of the quadrupolar relaxation from the low symmetry 35Cl nucleus with the paramagnetic metal centre resulting in broad 1H and 35Cl NMR signals. However, dipolar 35Cl NMR chemical shifts induced by the addition of chloride to axially symmetric [Ln(DOTA)]− complexes give well-resolved 35Cl NMR spectra that can be interpreted as evidence of interaction with chloride.36 By contrast, when [Tb(pDO3A)] was added to a solution of KCl in deuterium oxide, no new peaks were observed in 35Cl NMR, and the chemical shift of the chloride resonance was unchanged, suggesting that chloride does not bind in our model system (Fig. S45‡).
The 35Cl NMR spectra of [Tb2(DO3A)2C-3] in deuterium oxide display chemical shift upon the addition of KCl (Fig. 2b). This shift can be ascribed to fast exchange between bound and free chloride; this is borne out by the fact that increasing addition of KCl increases the observed paramagnetic shift. Therefore, 35Cl NMR titrations were pursued with [Tb2(DO3A)2C-3] against KCl in D2O. The resulting chemical shifts were fitted to generate a binding isotherm. A strong first binding event followed by a very weak second binding event was observed (Fig. S47, S49, S51 and S52‡). Titrations were performed at 4 different temperatures in D2O in order to understand the thermodynamics of chloride binding to [Tb2(DO3A)2C-3] (Fig. S46–S52‡). The resulting van't Hoff plot suggested this chelation to be exothermic with high negative enthalpy (Fig. S53‡). By comparison with the results reported for [Tb(DOTA)]− where chloride binding is axial and a negative shift results (Fig. S45‡),36 this suggests that chloride ions bind at the equatorial position on the metal centres in [Tb2(DO3A)2C-3] (Fig. 2). Similarly, 35Cl NMR titrations were performed with [Tb2(DO3A)2C-2] against KCl in D2O at 4 different temperatures. Although chlorine bound chemical shifts were observed, the resulting binding isotherms were sigmoidal in shape which was difficult in deducing meaningful binding events. However, they suggest the likely competition between chloride and hydroxide in occupying the binding site between the metal centres in [Tb2(DO3A)2C-2].
After establishing chloride binding by the binuclear Eu(III) and Tb(III) complexes in water, the association was further evaluated by high resolution ESI-Mass spectrometry. The mass spectral peak of a chloride bound to the Eu(III) binuclear complexes in deionised water were found at m/z 1051.1486 and m/z 1065.1640 for C-2 and C-3 complexes, respectively, and confirmed by the calculated isotopic distribution pattern (Fig. S54 and S55‡), thus further supporting the formation of the ternary complexes [Ln2(DO3A)2C-2(μ-Cl)]− and [Ln2(DO3A)2C-3(μ-Cl)]−.
Steady-state emission titrations revealed that three fluoride ions are successively bound to the binuclear lanthanide complexes as the fluoride concentration was increased in deionised water. These three binding events were also observed in methanol, where the experimental observables at each event were better resolved, presumably due to better solvation of KF, and the lack of competing hydroxides.39 The binding isotherms were fitted to three binding events; all three were needed to generate an acceptable fit (Fig. 3).
Fig. 3 (a) Steady-state emission titration spectra of 1 mM [Eu2(DO3A)2C-2] against KF (stock concentration, 0.02 M) in deionised water at 22 °C. Spectrum of neat complex solution ( in bold), spectra upon the additions of KF ( to ), spectrum upon the final addition of KF ( in bold) (non-dilution method used). The inset expands the ΔJ = 0 and ΔJ = 1 emission bands and the asterisks highlight the emission maxima used in quantifying the binding of fluoride to the complex (Fig. S79 for binding isotherm‡). (b) Normalised trend of selected emission wavelengths in ΔJ = 0 and ΔJ = 1 transitions obtained from the titration of [Eu2(DO3A)2C-2] against KF in deionised water at 22 °C used in studying and quantifying binding. (c) Normalised model of speciation obtained from 580 nm emission in the steady-state emission titration spectra of [Eu2(DO3A)2C-2] against KF in deionised water at 22 °C. |
From the luminescence titrations (Fig. 3, S72, S73 and S79‡ for [Eu2(DO3A)2C-2]; Fig. S84, S85, S92, and S93‡ for [Eu2(DO3A)2C-3]), it can be hypothesised that the speciation involves binding of first fluoride (K1) by chelation between the metal centres. Excess addition of KF generates the second binding event (K2) which involves chelation of fluoride to each metal, while the third binding event (K3) forms a bridging fluoride in addition to the fluoride chelated to each metal (Fig. 4).
Fig. 4 Fluoride chelation by the binuclear complexes in aqueous media. (a) Structural representation of binding events in aqueous media. (b) Stacked steady-state luminescence of 1 mM [Eu2(DO3A)2C-2] with KF in methanol at 22 °C. The spectra are arranged as per the binding events deduced from the luminescence titration spectra (Fig. S72‡) and binding isotherm (Fig. S73‡). (c) Stacked steady-state luminescence of 1 mM [Eu2(DO3A)2C-3] with KF in methanol at 22 °C. The spectra are arranged as per the binding events deduced from the luminescence titration spectra (Fig. S92‡) and binding isotherm (Fig. S93‡). (d) 500 MHz stacked paramagnetic 1H NMR spectra of [Yb2(DO3A)2C-2] with increasing KF in deuterium oxide at 298 K. (e) 500 MHz stacked paramagnetic 1H NMR spectra of [Yb2(DO3A)2C-3] with increasing KF in deuterium oxide at 298 K. |
When titrations with the binuclear Eu(III) complexes and KF were performed in competing (phosphate buffered saline at pH 7.4), non-competing (Tris–HCl buffer at pH 7.4), and basic (CHES buffer at pH 9.98) media, the binding strength as well as the number of fluoride bound to the binuclear Eu(III) complexes were lowered and no more than two binding events were observed (Fig. S66–S71‡ for [Eu2(DO3A)2C-2] and Fig. S84–S91‡ for [Eu2(DO3A)2C-3]). A single crystal X-ray structure of [Yb2(DO3A)2C-3(2F)]2− was obtained (Fig. 5) which verifies our hypothesis on K2 mode of fluoride binding to the binuclear complexes. In luminescence titrations, the emission spectral change caused by fluoride is so high due to its strong influence on the crystal-filed of the metal centre as a result of its small-size with highly dense charge and strong electrostatic interaction in comparison with chloride.16d,29a–c It is noteworthy from the above observations that although fluoride chelation by the binuclear systems suffers from competing ions in buffers, chloride binding is enhanced amidst competition from other ions (Table 2).
Fig. 5 Single crystal X-ray of [Yb2(DO3A)2C-3(2F)]2−. H atoms and water omitted for clarity. Thermal ellipsoid drawn at 30% probability level. |
As expected, in luminescence lifetime measurements on the binuclear Eu(III) complexes, upon increasing the concentration of fluoride in deionised water, methanol and their deuterated counterparts, a decrease in the hydration number accounting for the displacement of inner-sphere water by the coordination of fluoride ions was observed (Fig. S110, S111, S113 and S114; Tables S2, S3, S5 and S6‡). Surprisingly, no change in the luminescence lifetime was observed during the addition of chloride with Eu(III) complexes which we hypothesise due to a counteracting interference between Photoinduced electron transfer (PeT) from chloride and intermetallic luminescence quenching.
The 1H NMR spectra of Eu(III) and Yb(III) binuclear complexes sharpen with increasing addition of fluoride due to its chelation involving both the metal centres which slows the rate of interconversion between the SAP and TSAP isomers (Fig. 4d, e, S27, S29, S30, S32, S33, S35 and S37‡). New signals are observed that extend the NMR spectral range in both the positive and negative chemical shift regions suggesting equatorial binding of fluoride with respect to the metal centre: axial binding of fluoride commonly results in a decrease or inversion of the local crystal field by destabilising axially oriented mj states, while equatorial binding destabilises other mj states.27–2919F NMR spectra of binuclear Eu(III) complexes in deuterium oxide contain a small peak at around −450 ppm for the fluoride bound to the complexes (Fig. S42 and S43‡) which is similar to the chemical shift reported for fluoride binding in mononuclear complexes.27d,28,29
Footnotes |
† This manuscript is dedicated to Prof. David Parker on his retirement from the University of Durham. |
‡ Electronic supplementary information (ESI) available: Detailed methods and materials, detailed synthesis and characterisation, titrations (NMR and luminescence), speciation models, luminescence lifetimes, and single crystal X-ray data. CCDC 2201928–2201934. For ESI and crystallographic data in CIF or other electronic format see DOI: https://doi.org/10.1039/d2sc05417e |
§ Hofmeister series of anion hydrophobicity (taken from ref. 17): CO32− > SO42− > S2O32− > H2PO4− > HO− > F− > HCO2− > CH3CO2− > Cl− > Br− > NO3− > I− > CIO4− > SCN−. |
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